The Konishi anomaly occurs in gauge theories incorporating this, and renormalizable couplings in theories incorporating it do not violate R-parity. Adding this theory to quantum mechanics allows analyzing systems using partner Hamiltonians, which have corresponding eigenstates. Adding it in a namesake minimal extension of the (*) standard model creates the phenomenon of gauge coupling unification, in which makes the strong, weak, and electromagnetic forces approximately equal at high energies, solving the hierarchy problem. Postulated by Murayama, Zumino, Wess, and several others, this theory predicts the existence of charginos, gluinos, grav
The Konishi anomaly occurs in gauge theories incorporating this, and renormalizable couplings in theories incorporating it do not violate R-parity. Adding this theory to quantum mechanics allows analyzing systems using partner Hamiltonians, which have corresponding eigenstates. Adding it in a namesake minimal extension of the (*) standard model creates the phenomenon of gauge coupling unification, in which makes the strong, weak, and electromagnetic forces approximately equal at high energies, solving the hierarchy problem. Postulated by Murayama, Zumino, Wess, and several others, this theory predicts the existence of charginos, gluinos, gravitinos, and the like, and this theory postulates that the lightest possible partner comprises dark matter. FTP, name this theory, which pairs every observed particle with another one that differs by spin one half.
The Konishi anomaly occurs in gauge theories incorporating this, and renormalizable couplings in theories incorporating it do not violate R-parity.
{Supersymmetry} or {SUSY} [do not accept "{String theory}"]